Particle dynamics and pair production in tightly focused standing wave

With the advent of 10 PW laser facilities, new regimes of laser-matter interaction are opening since effects of quantum electrodynamics, such as electron-positron pair production and cascade development, start to be important. The dynamics of light charged particles, such as electrons and positrons, is affected by the radiation reaction force. This effect can strongly influence the interaction of intense laser pulses with matter since it lowers the energy of emitting particles and transforms their energy to the gamma radiation. Consequently, electron-positron pairs can be generated via Breit-Wheeler process. To study this new regime of interaction, numerical simulations are required. With their help it is possible to predict and study quantum effects which may occur in future experiments at modern laser facilities. In this work we present results of electron interaction with an intense standing wave formed by two colliding laser pulses. Due to the necessity to achieve ultra intense laser field, the laser beam has to be focused to a ~μm-diameter spot. Since the paraxial approximation is not valid for tight focusing, the appropriate model describing the tightly focused laser beam has to be employed. In tightly focused laser beam the longitudinal component of the electromagnetic field becomes significant and together with the ponderomotive force they affect the dynamics of interacting electrons and also newly generated Breit-Wheeler electron-positron pairs. Using the Particle-In-Cell code we study electron dynamics, gamma radiation and pair production in such a configuration for linear polarization and different types of targets.

[1]  Thomas Grismayer,et al.  Electron–positron cascades in multiple-laser optical traps , 2016, 1609.08081.

[2]  Kenneth W. D. Ledingham,et al.  Laser-driven particle and photon beams and some applications , 2010 .

[3]  V. I. Ritus Quantum effects of the interaction of elementary particles with an intense electromagnetic field , 1985 .

[4]  Matteo Tamburini,et al.  Laser-pulse-shape control of seeded QED cascades , 2015, Scientific Reports.

[5]  J. Vieira,et al.  Modelling radiation emission in the transition from the classical to the quantum regime , 2015, 1507.08607.

[6]  A M Fedotov,et al.  Limitations on the attainable intensity of high power lasers. , 2010, Physical review letters.

[7]  G. Breit,et al.  Collision of Two Light Quanta , 1934 .

[8]  S. V. Bulanov,et al.  Schwinger limit attainability with extreme power lasers. , 2010, Physical review letters.

[9]  Yousef I. Salamin Fields and propagation characteristics in vacuum of an ultrashort tightly focused radially polarized laser pulse , 2015 .

[10]  Hans A. Bethe,et al.  On the Stopping of Fast Particles and on the Creation of Positive Electrons , 1934 .

[11]  R. Fonseca,et al.  Seeded QED cascades in counterpropagating laser pulses. , 2015, Physical review. E.

[12]  Yasuhiko Sentoku,et al.  Higher order terms of radiative damping in extreme intense laser-matter interaction , 2012 .

[13]  Georg Korn,et al.  Attractors and chaos of electron dynamics in electromagnetic standing waves , 2014, Physics Letters A.

[14]  M. Marklund,et al.  Depletion of Intense Fields. , 2016, Physical review letters.

[15]  Julian Schwinger,et al.  On gauge invariance and vacuum polarization , 1951 .

[16]  K. Bennett,et al.  Modelling gamma-ray photon emission and pair production in high-intensity laser-matter interactions , 2013, J. Comput. Phys..

[17]  J. G. Kirk,et al.  Pair production in counter-propagating laser beams , 2009, 0905.0987.

[18]  Christoph H. Keitel,et al.  Fields of an ultrashort tightly focused laser pulse , 2015, 1504.00988.

[19]  Pascal Monot,et al.  Design and current progress of the Apollon 10 PW project , 2014, High Power Laser Science and Engineering.

[20]  T. Arber,et al.  Dense electron-positron plasmas and ultraintense γ rays from laser-irradiated solids. , 2012, Physical review letters.

[21]  G. Mourou,et al.  Ultra-high intensity-high contrast 300-TW laser at 0.1 Hz repetition rate , 2008, 2008 Conference on Lasers and Electro-Optics and 2008 Conference on Quantum Electronics and Laser Science.

[22]  E. N. Nerush,et al.  Optimized multibeam configuration for observation of QED cascades , 2015, 1505.06680.